A. Bartolo, N. Vigne, M. Marconi, G. Beaudoin, K. Pantzas, I. Sagnes, A. Garnache, M. Giudici
{"title":"简并光腔中时间局域结构的空间复用","authors":"A. Bartolo, N. Vigne, M. Marconi, G. Beaudoin, K. Pantzas, I. Sagnes, A. Garnache, M. Giudici","doi":"10.1109/CLEO/Europe-EQEC57999.2023.10232687","DOIUrl":null,"url":null,"abstract":"Temporal localized structures (TLS) are individually addressable pulses circulating in an optical cavity [1]. Their existence is related to the presence of a generalized multistability between pulsating emission states having different number of pulses per roundtrip. They appear in passively mode-locked Vertical External-Cavity Surface-Emitting Lasers (VECSELs) when i) the cavity roundtrip $(\\tau_{\\mathrm{c}})$ is larger than the carrier recovery time (typically 1 ns) and ii) the saturable absorber mirror (SESAM) exhibits a modulation depth above a critical value (typically 8%) [2], [3]. When the external cavity is nearly degenerate, i.e. close to self-imaging condition, temporal-localized patterns are observed [4]. On the other hand, degenerate cavities enable arbitrary spatial shaping of the lasing emission profile [5].","PeriodicalId":19477,"journal":{"name":"Oceans","volume":"0704 1","pages":"1-1"},"PeriodicalIF":0.0000,"publicationDate":"2023-06-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Spatial Multiplexing of Temporal Localized Structures in Degenerate Optical Cavities\",\"authors\":\"A. Bartolo, N. Vigne, M. Marconi, G. Beaudoin, K. Pantzas, I. Sagnes, A. Garnache, M. Giudici\",\"doi\":\"10.1109/CLEO/Europe-EQEC57999.2023.10232687\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Temporal localized structures (TLS) are individually addressable pulses circulating in an optical cavity [1]. Their existence is related to the presence of a generalized multistability between pulsating emission states having different number of pulses per roundtrip. They appear in passively mode-locked Vertical External-Cavity Surface-Emitting Lasers (VECSELs) when i) the cavity roundtrip $(\\\\tau_{\\\\mathrm{c}})$ is larger than the carrier recovery time (typically 1 ns) and ii) the saturable absorber mirror (SESAM) exhibits a modulation depth above a critical value (typically 8%) [2], [3]. When the external cavity is nearly degenerate, i.e. close to self-imaging condition, temporal-localized patterns are observed [4]. On the other hand, degenerate cavities enable arbitrary spatial shaping of the lasing emission profile [5].\",\"PeriodicalId\":19477,\"journal\":{\"name\":\"Oceans\",\"volume\":\"0704 1\",\"pages\":\"1-1\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2023-06-26\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Oceans\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/CLEO/Europe-EQEC57999.2023.10232687\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Oceans","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CLEO/Europe-EQEC57999.2023.10232687","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Spatial Multiplexing of Temporal Localized Structures in Degenerate Optical Cavities
Temporal localized structures (TLS) are individually addressable pulses circulating in an optical cavity [1]. Their existence is related to the presence of a generalized multistability between pulsating emission states having different number of pulses per roundtrip. They appear in passively mode-locked Vertical External-Cavity Surface-Emitting Lasers (VECSELs) when i) the cavity roundtrip $(\tau_{\mathrm{c}})$ is larger than the carrier recovery time (typically 1 ns) and ii) the saturable absorber mirror (SESAM) exhibits a modulation depth above a critical value (typically 8%) [2], [3]. When the external cavity is nearly degenerate, i.e. close to self-imaging condition, temporal-localized patterns are observed [4]. On the other hand, degenerate cavities enable arbitrary spatial shaping of the lasing emission profile [5].